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FOUNDATIONS OF QUANTUM MECHANICS

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I. 2. INCOMPLETENESS AND LOCALITY 15<br />

by ‘influence’ the ‘defining effect’ of the context of measurement. The experimental circumstances<br />

define what you may call physical reality. Physical reality is not defined by experiments you could do,<br />

as is the case according to EPR, but exclusively by experiments you actually do. Under circumstances<br />

as described in the EPR experiment this ‘defining effect’ of the experimental setup also reaches parts<br />

of the system with which the measuring apparatus has no physical interaction.<br />

A distinct difference between Einstein and Bohr is that Einstein wants to visualize reality independent<br />

of observation, whereas Bohr is satisfied with complementary pictures of which the applicability<br />

always remains dependent on the chosen measurement setup. In 1955 Einstein says (Fine 1986, p.95)<br />

It is basic for physics that one assumes a real world existing independently from any act<br />

of perception. But this we do not know. We take it only as a programme in our scientific<br />

endeavors. This programme is, of course, prescientific and our ordinary language is<br />

already based on it.<br />

And concerning the EPR situation he says (Schilpp 1949, p. 85)<br />

But on one supposition we should, in my opinion, absolutely hold fast: the real factual<br />

situation of the system S 2 is independent of what is done with the system S 1 , which is<br />

spatially separated from the former.<br />

Bohr’s conceptions concerning physical reality are much more difficult to characterize. According<br />

to him there is no independent reality of which the physical theory would have to give an unambiguous<br />

representation. He writes (Schilpp 1949, p. 211)<br />

Thus, a sentence like “we cannot know both the momentum and the position of an atomic<br />

object” immediately raises questions as to the physical reality of two such attributes of the<br />

object, which can be answered only by referring to the conditions for the unambiguous<br />

use of space - time concepts, on the one hand, and dynamical conservation laws, on the<br />

other hand.<br />

An exhaustive description of reality must always use concepts which themselves remain dependent<br />

on mutually excluding contexts. Bohr says (A. Petersen 1963, p. 11)<br />

The word ‘reality’ is also a word, a word which we must learn to use correctly.<br />

He constantly emphasizes the restricted applicability of our physical concepts, which makes the link<br />

between description and reality very complicated. Petersen mentions (ibid., p. 12)<br />

When asked whether the algorithm of quantum mechanics could be considered as somehow<br />

mirroring an underlying quantum world, Bohr would answer, “There is no quantum<br />

world. There is only an abstract quantum physical description. It is wrong to think that<br />

the task of physics is to find out how nature is. Physics concerns what we can say about<br />

nature.”

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